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What is the energy of the orbiting electron in a hydrogen atom with a radial quantum number of \(45 ?\)

Short Answer

Expert verified
Answer: The energy of an electron in a hydrogen atom with a radial quantum number of 45 is approximately -6.42 x 10^-3 eV.

Step by step solution

01

Understand the energy equation of a hydrogen atom

The energy of an electron in a hydrogen atom depends on the principal quantum number (n) and it follows a formula: $$ E_n = -\frac{13.6 \ \text{eV}}{n^2}, \quad n \in \{1,2,3, ...\} $$ This equation helps us find the energy level at which the electron resides, given its principal quantum number. The negative sign represents that the energy of electron in an atom is less than zero, i.e., the electron is bound to the nucleus. Here, we are given the radial quantum number (45). To solve the problem, we must find the corresponding principal quantum number (n) first and then find the energy using the above formula.
02

Determine the principal quantum number (n) from the radial quantum number

In a hydrogen atom, we can determine the principal quantum number (n) by simply adding 1 to the radial quantum number: $$ n = l + 1 $$ Given the radial quantum number \(l = 45\), we can find the principal quantum number using the expression above: $$ n = 45 + 1 = 46 $$
03

Calculate the energy of the orbiting electron

Now that we have the principal quantum number (n = 46), we can use the energy equation for the hydrogen atom to find the energy of the orbiting electron. Plugging \(n = 46\) into the equation, we get: $$ E_{46} = -\frac{13.6 \ \text{eV}}{46^2} = -\frac{13.6 \ \text{eV}}{2116} \approx -6.42 \times 10^{-3} \ \text{eV} $$ The energy of the orbiting electron in a hydrogen atom with a radial quantum number of 45 is approximately \(-6.42 \times 10^{-3}\) eV.

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Most popular questions from this chapter

The binding energy of an extra electron added when As atoms are used to dope a Si crystal may be approximately calculated by considering the Bohr model of a hydrogen atom. a) Express the ground energy of the hydrogen-like atoms in terms of the dielectric constant, the effective mass of an extra electron, and the groundstate energy of a hydrogen atom. b) Calculate the binding energy of the extra electron in a Si crystal. The dielectric constant of \(\mathrm{Si}\) is about \(10.0,\) and the effective mass of extra electrons in a Si crystal is about \(20.0 \%\) of that of free electrons.

An excited hydrogen atom emits a photon with an energy of \(1.133 \mathrm{eV}\). What were the initial and final states of the hydrogen atom before and after emitting the photon?

The radius of the \(n=1\) orbit in the hydrogen atom is \(a_{0}=0.053 \mathrm{nm}\) a) Compute the radius of the \(n=6\) orbit. How many times larger is this than the \(n=1\) radius? b) If an electron in the \(n=6\) orbit drops to the \(n=1\) orbit (ground state), what are the frequency and the wavelength of the emitted radiation? What kind of radiation is emitted (visible, infrared, etc.)? c) How would your answer to part (a) change if the atom was a singly ionized helium atom (He \(^{+}\) ) instead?

Which model of the hydrogen atom-the Bohr model or the quantum mechanical model-predicts that the electron spends more time near the nucleus?

An electron in a hydrogen atom is in the \(2 s\) state. Calculate the probability of finding the electron within a Bohr radius \(\left(a_{0}=0.05295 \mathrm{nm}\right)\) of the proton. The \(2 s\) wave function for hydrogen is $$ \psi_{2 s}(r)=\frac{1}{4 \sqrt{2 \pi a_{0}^{3}}}\left(2-\frac{r}{a_{0}}\right) e^{-r / 2 a_{0}} $$ Evaluating the integral is a bit tedious, so you may want to consider using a program such as Mathcad or Mathematica or finding the integral online at http://integrals.wolfram.com/index.jsp.

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